12
12

Sep 22, 2013
09/13

by
Andrei A. Galiautdinov

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12

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Using the recently discovered Clifford statistics we propose a simple model for the grand canonical ensemble of the carriers in the theory of fractional quantum Hall effect. The model leads to a temperature limit associated with the permutational degrees of freedom of such an ensemble. We also relate Schur's theory of projective representations of the permutation groups to physics, and remark on possible extensions of the second quantization procedure.

Source: http://arxiv.org/abs/hep-th/0201052v3

3
3.0

Sep 18, 2013
09/13

by
David R. Finkelstein; Andrei A. Galiautdinov

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3

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0

At higher energies the present complex quantum theory with its unitary group might expand into a real quantum theory with an orthogonal group, broken by an approximate $i$ operator at lower energies. Implementing this possibility requires a real quantum double-valued statistics. A Clifford statistics, representing a swap (12) by a difference $\gamma_1-\gamma_2$ of Clifford units, is uniquely appropriate. Unlike the Maxwell-Boltzmann, Fermi-Dirac, Bose-Einstein, and para- statistics, which are...

Source: http://arxiv.org/abs/hep-th/0005039v2

37
37

Sep 22, 2013
09/13

by
Andrei A. Galiautdinov; David R. Finkelstein

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37

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0

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1

The Dirac equation is not semisimple. We therefore regard it as a contraction of a simpler decontracted theory. The decontracted theory is necessarily purely algebraic and non-local. In one simple model the algebra is a Clifford algebra with 6N generators. The quantum imaginary $\hbar i$ is the contraction of a dynamical variable whose back-reaction provides the Dirac mass. The simplified Dirac equation is exactly Lorentz invariant but its symmetry group is SO(3,3), a decontraction of the...

( 1 reviews )

Source: http://arxiv.org/abs/hep-th/0106273v2

14
14

Jul 20, 2013
07/13

by
David R. Finkelstein; Andrei A. Galiautdinov; James E. Baugh

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14

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Unimodular relativity is a theory of gravity and space-time with a fixed absolute space-time volume element, the modulus, which we suppose is proportional to the number of microscopic modules in that volume element. In general relativity an arbitrary fixed measure can be imposed as a gauge condition, while in unimodular relativity it is determined by the events in the volume. Since this seems to break general covariance, some have suggested that it permits a non-zero covariant divergence of the...

Source: http://arxiv.org/abs/gr-qc/0009099v1